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[PDF] Top 20 Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector

Has 10000 "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector" found on our website. Below are the top 20 most common "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector".

Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector

Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector

... SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, United Kingdom; DOE and NSF, United States of ...America. In addition, individual ... See full document

52

Search for heavy quarks decaying into a top quark and a $W$ or $Z$ boson using lepton + jets events in $pp$ collisions at $\sqrt{s}$ = 7 TeV

Search for heavy quarks decaying into a top quark and a $W$ or $Z$ boson using lepton + jets events in $pp$ collisions at $\sqrt{s}$ = 7 TeV

... tt+jets, W+jets, and Z+jets, are simulated using the M AD G RAPH ...[12] with CTEQ6L1 [13] parton distribution functions (PDF). The single top quark ... See full document

29

Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... consistent with originating from hadronic decays of W or Z ...background jets inside a mass window including the W / Z mass is based on the variable D ... See full document

23

Search for Dark Matter Produced in Association with a Higgs Boson Decaying to $b\bar b$ using 36 fb$^{-1}$ of $pp$ collisions at $\sqrt s=13$ TeV with the ATLAS Detector

Search for Dark Matter Produced in Association with a Higgs Boson Decaying to $b\bar b$ using 36 fb$^{-1}$ of $pp$ collisions at $\sqrt s=13$ TeV with the ATLAS Detector

... FIG. 1. Distributions of the invariant mass of the Higgs boson candidates m h ¼ m jj ; m J with two b tags in the SR for the four E miss ... See full document

21

Search for vector-boson resonances decaying to a top quark and bottom quark in the lepton plus jets final state in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

Search for vector-boson resonances decaying to a top quark and bottom quark in the lepton plus jets final state in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

... P. Vankov 118 , R. Vari 70a , E.W. Varnes 7 , C. Varni 53b , 53a , T. Varol 41 , D. Varouchas 128 , K.E. Varvell 154 , G.A. Vasquez 144b , J.G. Vasquez 180 , F. Vazeille 37 , D. Vazquez Furelos 14 , T. Vazquez Schroeder ... See full document

24

Search for heavy lepton resonances decaying to a $Z$ boson and a lepton in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

Search for heavy lepton resonances decaying to a $Z$ boson and a lepton in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

... three or more lepton candidates can be classified into two categor- ...ies. The first category consists of events with three prompt leptons produced in the decays ... See full document

37

Search for a new resonance decaying to a W or Z boson and a Higgs boson in the $\ell \ell / \ell \nu / \nu \nu + b \bar{b}$ final states with the ATLAS detector

Search for a new resonance decaying to a W or Z boson and a Higgs boson in the $\ell \ell / \ell \nu / \nu \nu + b \bar{b}$ final states with the ATLAS detector

... For the 2-lepton channel in the eeb¯b final state, the MJ background shape is determined by selecting events with reversed electron isolation criteria and its ... See full document

30

Search for new resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $\ell^+ \ell^- b\bar b$, $\ell \nu b\bar b$, and $\nu\bar{\nu} b\bar b$ channels with $pp$ collisions at $\sqrt s = 13$ TeV with the ATLAS detector

Search for new resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $\ell^+ \ell^- b\bar b$, $\ell \nu b\bar b$, and $\nu\bar{\nu} b\bar b$ channels with $pp$ collisions at $\sqrt s = 13$ TeV with the ATLAS detector

... 2.0. The calorimeter system covers the pseudorapidity range |η| < ...composed of sampling calorimeters with either liquid argon or scintillator tiles as the active ...media. ... See full document

36

Search for Higgs bosons produced via vector-boson fusion and decaying into bottom quark pairs in $\sqrt{s} = 13$ $\mathrm{TeV}$ $pp$ collisions with the ATLAS detector

Search for Higgs bosons produced via vector-boson fusion and decaying into bottom quark pairs in $\sqrt{s} = 13$ $\mathrm{TeV}$ $pp$ collisions with the ATLAS detector

... Following the discovery of a new particle with a mass of 125 GeV by the ATLAS and CMS Collaborations at the Large Hadron Collider (LHC) [1,2] , there has been an ... See full document

29

Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

... ¼ 13 TeV. The data set corresponds to an integrated luminosity of ...36.1 fb1 . This analysis selects events with exactly two opposite-charge muons and classifies ... See full document

20

Search for an invisibly decaying Higgs boson or dark matter candidates produced in association with a $Z$ boson in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

Search for an invisibly decaying Higgs boson or dark matter candidates produced in association with a $Z$ boson in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

... examine the compatibility of the data and the signal-plus-background hypothesis, a test statistic is defined using the profile likelihood ratio method [ 84 ...]. The ... See full document

35

Search for invisible decays of the Higgs boson produced in association with a hadronically decaying vector boson in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

Search for invisible decays of the Higgs boson produced in association with a hadronically decaying vector boson in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

... for Higgs boson decays to invisible particles (H → ...both the ATLAS and CMS collaborations [ 14 , 19 ...example, the ATLAS Collaboration has placed an upper limit ... See full document

35

Search for the standard model Higgs boson produced in association with top quarks and decaying into a $b\bar{b}$ pair in $pp$ collisions at $\sqrt{s}$ = 13  TeV with the ATLAS detector

Search for the standard model Higgs boson produced in association with top quarks and decaying into a $b\bar{b}$ pair in $pp$ collisions at $\sqrt{s}$ = 13  TeV with the ATLAS detector

... using the anti-k t algorithm with a radius parameter R ¼ 0.4, and are required to have p T > 15 GeV and jηj < ...than the one described in Sec. III . The flavor ... See full document

44

Search for a new heavy gauge boson resonance decaying into a lepton and missing transverse momentum in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS experiment

Search for a new heavy gauge boson resonance decaying into a lepton and missing transverse momentum in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS experiment

... from W → `ν, Z/γ ∗ → ``, W → τν, and Z/γ ∗ → ττ were simulated using the Powheg- Box v2 [ 11 ] matrix-element calculation up to next-to-leading order (NLO) in perturbative ... See full document

33

Search for the Standard Model Higgs boson produced in association with top quarks and decaying into $b\bar{b}$ in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

Search for the Standard Model Higgs boson produced in association with top quarks and decaying into $b\bar{b}$ in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

... After the event selection described above, the main background in both the single-lepton and dilepton chan- nels is t¯ t+jets ...production. In the single-lepton ... See full document

52

Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at $ \sqrt{s}=8 $ TeV

Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at $ \sqrt{s}=8 $ TeV

... theories of physics beyond the standard model (SM) predict the existence of vector reso- nances with masses above 1 TeV that decay into a W or ... See full document

40

Search for a multi-Higgs-boson cascade in $W^+W^−b\bar{b}$ events with the ATLAS detector in pp collisions at $\sqrt{s} = 8$  TeV

Search for a multi-Higgs-boson cascade in $W^+W^−b\bar{b}$ events with the ATLAS detector in pp collisions at $\sqrt{s} = 8$  TeV

... A search is presented for new particles in an extension to the Standard Model that includes a heavy Higgs boson (H 0 ), an intermediate charged Higgs boson pair (H ... See full document

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Search for heavy resonances decaying to a photon and a hadronically decaying $Z/W/H$ boson in $pp$ collisions at $\sqrt{s}=13$ $\mathrm{TeV}$ with the ATLAS detector

Search for heavy resonances decaying to a photon and a hadronically decaying $Z/W/H$ boson in $pp$ collisions at $\sqrt{s}=13$ $\mathrm{TeV}$ with the ATLAS detector

... microstrip and transition radiation tracking detectors, covers the pseudorapidity 1 range |η| < ...2.5. The energies of photons and jets are measured primarily by ... See full document

44

Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... E.L. Gkougkousis 14 , P. Gkountoumis 10 , L.K. Gladilin 111 , C. Glasman 96 , J. Glatzer 14 , P.C.F. Glaysher 46 , A. Glazov 46 , M. Goblirsch-Kolb 26 , J. Godlewski 42 , S. Goldfarb 102 , T. Golling 55 , D. ... See full document

23

Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at $ \sqrt{s}=13 $ TeV

Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at $ \sqrt{s}=13 $ TeV

... normalization of the simulated top quark background is corrected with a scale factor de- termined in eight dedicated control regions, defined by inverting one selection criteria and ... See full document

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